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JPH0320053B2 - - Google Patents
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JPH0320053B2 - - Google Patents

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Publication number
JPH0320053B2
JPH0320053B2 JP61099938A JP9993886A JPH0320053B2 JP H0320053 B2 JPH0320053 B2 JP H0320053B2 JP 61099938 A JP61099938 A JP 61099938A JP 9993886 A JP9993886 A JP 9993886A JP H0320053 B2 JPH0320053 B2 JP H0320053B2
Authority
JP
Japan
Prior art keywords
permanent magnet
magnetic
magnetic field
yoke
air gap
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP61099938A
Other languages
Japanese (ja)
Other versions
JPS62256416A (en
Inventor
Takanobu Myamoto
Hideya Sakurai
Hirobumi Takabayashi
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Proterial Ltd
Original Assignee
Sumitomo Special Metals Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sumitomo Special Metals Co Ltd filed Critical Sumitomo Special Metals Co Ltd
Priority to JP61099938A priority Critical patent/JPS62256416A/en
Priority to US06/909,327 priority patent/US4679022A/en
Priority to EP86307272A priority patent/EP0228154B1/en
Priority to DE8686307272T priority patent/DE3676066D1/en
Publication of JPS62256416A publication Critical patent/JPS62256416A/en
Publication of JPH0320053B2 publication Critical patent/JPH0320053B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 産業分野 この発明は、対象物の断面イメージを得て組織
の性質まで描き出すことのできる医療用核磁気共
鳴断層撮影装置(以下、NMR−CTという)に
用いられる永久磁石を使用した磁界発生装置に係
り、大きな空隙内に強力かつ高精度で均一な静磁
界を発生する磁界発生装置に関する。
[Detailed Description of the Invention] Industrial Field This invention relates to a permanent magnet used in a medical nuclear magnetic resonance tomography device (hereinafter referred to as NMR-CT) that can obtain a cross-sectional image of an object and depict the properties of the tissue. The present invention relates to a magnetic field generating device that generates a strong, highly accurate, and uniform static magnetic field within a large air gap.

背景技術 NMR−CTは、人体の一部または全部を1〜
10KGの強力な磁界を形成する空隙内に挿入して
所要の断層イメージを得るため、この磁界が強力
かつ10-4以下の精度で一様で安定していることが
要求され、NMR−CT用の磁界発生装置として
は、銅またはアルミニウムからなる導線を円筒状
に巻着した常伝導磁石あるいは、特殊な導線を用
い、絶対零度付近の温度に冷却して使用する超伝
導磁石が知られている。
BACKGROUND ART
In order to obtain the desired tomographic image by inserting the device into an air gap that generates a strong magnetic field of 10 KG, this magnetic field must be strong, uniform, and stable with an accuracy of 10 -4 or less. Known magnetic field generators include normal conducting magnets made of conductive wires made of copper or aluminum wrapped around them in a cylindrical shape, and superconducting magnets that use special conducting wires cooled to a temperature close to absolute zero. .

前者は構造上安価であるが十分な強力磁界を発
生させるためには、膨大な電力と冷却水が必要で
あり、ランニングコストが高い等の問題があり、
一方、後者の超伝導磁石は、電力の消費が少なく
小型で強力な磁界を発生し得る利点があるが、冷
媒として高価な液体ヘリウム等の使用が不可欠で
あり、いわゆるイニシヤルコストとともにランニ
ングコストも著しく高い問題がある。
The former is structurally inexpensive, but it requires a huge amount of electricity and cooling water to generate a sufficiently strong magnetic field, and has problems such as high running costs.
On the other hand, the latter type of superconducting magnet has the advantage of consuming less power and being able to generate a strong magnetic field in a small size, but it is essential to use expensive liquid helium as a coolant, which increases the running cost as well as the so-called initial cost. There are significant problems.

本出願人は、先に、磁界強度が上記の常伝導磁
石と同等以上で、ランニングコストが安く、超電
導磁石、常電導磁石に比べて、漏洩磁界の少ない
永久磁石を使用した磁界発生装置を提案(実願昭
59−53575号)した。
The applicant previously proposed a magnetic field generator using a permanent magnet, which has a magnetic field strength equal to or higher than that of the above-mentioned normal conducting magnet, has low running costs, and has less magnetic field leakage than superconducting magnets and normal conducting magnets. (Akira Jigan
No. 59-53575).

上記磁界発生装置は、第6図に示す如く、一対
の永久磁石構成体1,1の各々の一方端に磁極片
2,2を固着して対向させ、他方端を継鉄3で結
合し、磁極片2,2間の空隙内4に、静磁界を発
生させる構成であり、一対の磁極片2,2には、
その対向面の周縁に、所定の内径、高さからなる
断面略台形の環状突起5を突設し、さらに、磁極
片2,2の中央部に、所定径、高さからなる断面
略台形の凸状突起6を設けたからなり、空隙4内
に、強力かつ均一精度の高い磁界を発生する。
As shown in FIG. 6, the magnetic field generating device described above includes a pair of permanent magnet components 1, 1, with magnetic pole pieces 2, 2 fixed to one end of each of them facing each other, the other end of which is connected with a yoke 3, It is configured to generate a static magnetic field in the air gap 4 between the magnetic pole pieces 2, 2, and the pair of magnetic pole pieces 2, 2 include:
An annular protrusion 5 having a substantially trapezoidal cross section with a predetermined inner diameter and height is protruded from the periphery of the opposing surface, and an annular protrusion 5 having a substantially trapezoidal cross section with a predetermined inner diameter and height is provided at the center of the pole pieces 2, 2. A convex protrusion 6 is provided to generate a strong, uniform and highly accurate magnetic field within the air gap 4.

しかし、上記の磁界発生装置において、磁極か
らの磁束は空隙外に漏洩しやすく、空隙中心垂直
線上では、磁極面に近い程磁界強度が高くなる性
質があるため、使用磁界空間で所要の高い均一磁
界を得るためには、磁極間距離や磁極面積を大き
くするなど、使用磁界空間の数倍以上の空隙を要
し、磁界回路の小型化ができないという問題を有
していた。
However, in the above-mentioned magnetic field generator, the magnetic flux from the magnetic poles tends to leak out of the air gap, and on the vertical line of the air gap center, the closer to the magnetic pole surface the higher the magnetic field strength becomes. In order to obtain a magnetic field, it is necessary to increase the distance between the magnetic poles and the area of the magnetic poles, thereby creating an air gap several times larger than the magnetic field space to be used, which poses a problem in that the magnetic field circuit cannot be miniaturized.

発明の目的 この発明は、かかる現状に鑑み、所要空隙に高
精度で均一かつ安定な磁界を発生する磁界発生装
置において、均一磁界のより一層の拡大を計つた
磁界回路を有する磁界発生装置を目的とし、永久
構成体からの磁束を有効に集中させて、永久磁石
重量を低減して小型軽量化が達成できる磁界発生
装置を目的としている。
Purpose of the Invention In view of the current situation, the present invention aims to provide a magnetic field generating device that generates a highly accurate, uniform, and stable magnetic field in a required air gap, and that has a magnetic field circuit that further expands the uniform magnetic field. The purpose of the present invention is to provide a magnetic field generating device that can effectively concentrate the magnetic flux from the permanent structure, reduce the weight of the permanent magnet, and achieve a reduction in size and weight.

発明の構成と効果 この発明は、高精度で均一かつ安定な磁界が得
られ、かつ漏洩磁束の少ない磁気回路を目的に
種々検討した結果、一対の永久磁石構成体の磁極
面が、空隙に対して凹状湾曲面を形成するよう
に、平板状の永久磁石構成体の周囲に、別途の永
久磁石構成体を配置することにより、磁気回路空
隙内の磁界均一度及び磁界強度が著しく向上し、
高精度で均一な磁界域を拡大できることを知見し
たものである。
Structure and Effects of the Invention As a result of various studies aimed at creating a magnetic circuit that can obtain a highly accurate, uniform, and stable magnetic field and has little leakage magnetic flux, the present invention has been made based on the results that the magnetic pole surfaces of a pair of permanent magnet components are aligned with the air gap. By arranging a separate permanent magnet structure around the flat permanent magnet structure so as to form a concave curved surface, the magnetic field uniformity and magnetic field strength within the magnetic circuit gap are significantly improved.
This is based on the discovery that it is possible to expand the uniform magnetic field area with high precision.

すなわち、この発明は、 空隙を形成して対向する一対の永久磁石構成体
を継鉄で磁気的結合し、各永久磁石構成体の空隙
対向面に磁極片を固着し、該空隙に磁界を発生さ
せる磁界発生装置において、 平板状の中央部永久磁石と、 中央永久磁石の外周部に傾斜させて周設または
周配置する外周部永久磁石とにより、 磁極面に垂直方向に磁化された各対の永久磁石
磁極面が、空隙に対して凹状湾曲面を形成したこ
とを特徴とする磁界発生装置である。
That is, this invention magnetically couples a pair of permanent magnet structures facing each other by forming a gap with a yoke, fixes a magnetic pole piece to the surface of each permanent magnet structure facing the gap, and generates a magnetic field in the gap. In a magnetic field generating device, a flat central permanent magnet and an outer peripheral permanent magnet installed or arranged around the central permanent magnet in an inclined manner, each pair is magnetized in a direction perpendicular to the magnetic pole surface. This magnetic field generating device is characterized in that the permanent magnet magnetic pole surface forms a concave curved surface with respect to the air gap.

発明の好ましい実施態様 磁気回路は、空隙を形成して対向する一対の永
久磁石構成体を継鉄で磁気的結合すればいかなる
構成も利用でき、永久磁石構成体の磁気特性、形
状寸法、継鉄の形状寸法及び所要空隙の大きさ等
に応じて、永久磁石構成体の配置等を適宜選定す
ることが望ましい。
Preferred Embodiment of the Invention The magnetic circuit can have any configuration as long as a pair of opposing permanent magnet structures are magnetically coupled with a yoke by forming an air gap. It is desirable to appropriately select the arrangement of the permanent magnet structure, etc., depending on the shape and dimensions of the magnet, the size of the required air gap, etc.

磁気回路を構成する継鉄には、種々の構成、形
状のものが利用でき、例えば、第2図に示す継鉄
10は、一対の板状継鉄11,11を対向配置
し、複数(図では4本)の柱状継鉄12にて連結
した構成からなり、前記板状継鉄11,11の対
向する内面に、図示しないこの発明による永久磁
石構成体を着設すると、所要の空隙13が形成さ
れ、かかる空隙13には、いずれの方向の柱状継
鉄12間よりも、被診断対象物を挿入することが
できる利点があり、また、組立及び保守管理も容
易となる。
Various configurations and shapes can be used for the yoke constituting the magnetic circuit. For example, the yoke 10 shown in FIG. When a permanent magnet structure according to the present invention (not shown) is attached to the opposing inner surfaces of the plate yokes 11, 11, the required air gap 13 is formed. The gap 13 thus formed has the advantage that the object to be diagnosed can be inserted more easily than between the columnar yokes 12 in either direction, and assembly and maintenance management are also facilitated.

また、第2図では板状継鉄11,11に、正方
形板を用いた例を示したが、円板状など任意の形
状が適用でき、例えば、狭い場所への搬送、設置
等を考慮して長方形板を用いるものもよい。
In addition, although Fig. 2 shows an example in which square plates are used as the plate-shaped yokes 11, 11, any shape such as a disk shape can be applied. It is also good to use a rectangular plate.

さらに、柱状継鉄12は、自身を通る磁束が飽
和しない範囲で、その形状、本数等を選定するこ
とが望ましい。
Furthermore, it is desirable to select the shape, number, etc. of the columnar yoke 12 within a range that does not saturate the magnetic flux passing through it.

第3図に示す継鉄14は、円板状継鉄15,1
6を対向配置し、両者を円筒状継鉄17にて接続
した構成であり、対向する円板状継鉄15,16
内面に図示しない永久磁石構成体を着設して、空
隙を形成するが、該空隙が円筒状継鉄17にて包
囲される構成で、円筒状継鉄17に被診断対象物
を挿入するための開口部17aが設けられるだけ
で、継鉄14からの漏洩磁界がほとんどない利点
がある。
The yoke 14 shown in FIG.
6 are arranged facing each other, and both are connected by a cylindrical yoke 17, and the opposing disc-shaped yokes 15, 16
A permanent magnet structure (not shown) is attached to the inner surface to form a gap, and the gap is surrounded by the cylindrical yoke 17, in order to insert the object to be diagnosed into the cylindrical yoke 17. There is an advantage that there is almost no leakage magnetic field from the yoke 14 simply by providing the opening 17a.

第4図に示す継鉄18は、四角筒状継鉄で、開
口19方向を水平にし、上下の継鉄面18a,1
8bの内面に図示しない一対の永久磁石構成体を
着設し、空隙を形成する構成からなる。
The yoke 18 shown in FIG. 4 is a square cylindrical yoke, with the opening 19 directed horizontally, and the upper and lower yoke surfaces 18a, 1
A pair of permanent magnet structures (not shown) are attached to the inner surface of the magnet 8b to form a gap.

この発明において、上述の継鉄等、各種構成の
継鉄の対向継鉄面に、一対の永久磁石構成体を着
設するが、永久磁石構成体は、平板状の中央部永
久磁石と、中央永久磁石の外周部に傾斜させて周
設または周配置する外周部永久磁石とにより、凹
状磁極面を形成できれば、中央部永久磁石形状は
円板状、多角形状等種々形状が採用でき、外周部
永久磁石は中央永久磁石形状や空隙における所要
磁界均一度等に応じて、周設あるいは中央部永久
磁石中心から放射状位置に所要数を周配置するこ
ともよい。
In this invention, a pair of permanent magnet structures are attached to opposing yoke surfaces of yokes of various configurations, such as the above-mentioned yoke. If a concave magnetic pole surface can be formed by the outer periphery permanent magnet installed or arranged around the outer periphery of the permanent magnet at an angle, the shape of the central permanent magnet can be of various shapes such as a disk shape or a polygonal shape. Depending on the shape of the central permanent magnet, the required uniformity of the magnetic field in the gap, etc., the permanent magnets may be arranged around the circumference or in a required number at radial positions from the center of the central permanent magnet.

また、いずれの永久磁石も、通常、複数個のブ
ロツク状磁石を着磁組立法にて、所要形状に組立
るため、組立作業性を考慮した形状が望ましく、
例えば、中央部永久磁石を多角形状とし、その外
周各辺に当接し得る形状からなる外周部永久磁石
に配置する構成を取ると、永久磁石構成体の組立
が容易になる。
In addition, since all permanent magnets are usually assembled into a desired shape using a magnetization assembly method using a plurality of block-shaped magnets, it is desirable to have a shape that takes assembly workability into consideration.
For example, if the central permanent magnet is made into a polygonal shape and arranged in an outer peripheral permanent magnet having a shape that can come into contact with each side of the outer periphery, the permanent magnet assembly can be easily assembled.

この発明において、上述の如く、対向磁極面を
凹状湾曲面となした永久磁石構成体の磁極面に、
凹状湾曲面を有する磁極片を着設するが、磁極片
は、その空隙対向面が所要の均一磁界を考慮した
凹状湾曲面を構成すればよく、永久磁石に当接す
る裏面は、中央部永久磁石及び外周部永久磁石の
形状、個数などに応じた適宜選定する必要があ
る。
In this invention, as described above, on the magnetic pole surface of the permanent magnet structure in which the opposing magnetic pole surface is a concave curved surface,
A magnetic pole piece having a concave curved surface is installed, and the surface of the magnetic pole piece facing the air gap may form a concave curved surface considering the required uniform magnetic field, and the back surface that contacts the permanent magnet is attached to the central permanent magnet. It is necessary to select an appropriate value depending on the shape, number, etc. of the outer peripheral permanent magnet.

例えば、第5図に示す磁極片20は、所要の凹
状湾曲面を有する所謂深皿状からなり、その永久
磁石との当接面は、永久磁石構成体が8角形の中
央部永久磁石とその外周各辺に当接しかつ周方向
に相互隣接可能な台形状の外周部永久磁石で構成
されるのを考慮し、B図の底図面に示す如く、8
角形の平面部21と平面部21の外周部21の外
周に周設した8個の台形状傾斜部22から構成し
てあり、永久磁石構成体との確実な磁路形成を確
保している。
For example, the magnetic pole piece 20 shown in FIG. 5 has a so-called deep-dish shape with a required concave curved surface, and the contact surface with the permanent magnet is formed between the central permanent magnet whose permanent magnet structure is octagonal and its contact surface with the permanent magnet. Considering that it is composed of trapezoidal outer peripheral permanent magnets that contact each side of the outer periphery and can be adjacent to each other in the circumferential direction, as shown in the bottom drawing of Figure B, 8.
It is composed of a rectangular flat part 21 and eight trapezoidal inclined parts 22 provided around the outer periphery of the outer peripheral part 21 of the flat part 21, ensuring reliable magnetic path formation with the permanent magnet structure.

また、C図に示す如く、磁極片20の空隙対向
側平面部23の中央部に、突起部24を設けて、
空隙内の磁極均一度を向上させる構成とするのも
よい。
Further, as shown in Fig. C, a protrusion 24 is provided at the center of the plane portion 23 of the magnetic pole piece 20 on the side opposite to the air gap.
It is also possible to adopt a configuration that improves the uniformity of the magnetic poles within the air gap.

この発明の磁極発生装置に用いる永久磁石は、
フエライト磁石、アルニコ系磁石、希土類コバル
ト系磁石が使用できるが、先に出願人が提案(特
願昭57−145072号)した、RとしてNdやPrを中
心とする資源的に豊富な軽希土類を用い、B、
Feを主成分として25MGO8以上の極めて高いエ
ネルギー積を示す、Fe−B−R系永久磁石を使
用することにより、著しく小型化することができ
る。
The permanent magnet used in the magnetic pole generator of this invention is
Ferrite magnets, alnico-based magnets, and rare earth cobalt-based magnets can be used, but the applicant previously proposed (Japanese Patent Application No. 145072/1982) that R should be a light rare earth material that is rich in resources, mainly Nd and Pr. Use, B,
By using a Fe-BR-based permanent magnet that has Fe as its main component and exhibits an extremely high energy product of 25 MGO 8 or more, it can be significantly miniaturized.

図面に基づく発明の開示 第1図はこの発明による磁界発生装置に用いる
磁気回路の横断上面図とB−B断面図である。
DISCLOSURE OF THE INVENTION BASED ON THE DRAWINGS FIG. 1 is a cross-sectional top view and a BB sectional view of a magnetic circuit used in a magnetic field generating device according to the present invention.

磁気回路は、その継鉄30が、正方形からなる
一対の板状継鉄31,32を対向配置して4本の
円柱状継鉄33にて連結した構成からなり、前記
板状継鉄31,32の対向する内面に、この発明
による永久磁石構成体40,50を着設して、所
要の空隙60を形成してある。
In the magnetic circuit, the yoke 30 has a configuration in which a pair of square plate yokes 31 and 32 are arranged facing each other and connected by four cylindrical yokes 33, and the plate yokes 31, Permanent magnet structures 40, 50 according to the present invention are attached to the opposing inner surfaces of the magnets 32 to form the required air gap 60.

継鉄30は、下側の板状継鉄32の四隅に立設
された円柱状継鉄33が、上側の板状継鉄31の
四隅の穴部に貫通し、突出した円柱状継鉄33を
覆う有頭筒体のカバー34が、上側の板状継鉄3
1の穴部外周にボルト35で固着され、中央部に
螺合する調整ボルト36にて上側の板状継鉄31
が円柱状継鉄33の上端に載置され、調整ボルト
36の螺合進退により、上下に微動可能となした
上側の板状継鉄31は、その水平レベルあるいは
下側の板状継鉄32との対向距離を調整できる構
成であり、さらに調整ボルト36の周囲に設けた
固定ボルト37にて、カバー34と柱状継鉄33
とを固定できる構成である。
In the yoke 30, cylindrical yokes 33 erected at the four corners of the lower plate-shaped yoke 32 penetrate through holes at the four corners of the upper plate-shaped yoke 31, and the cylindrical yoke 33 protrudes. The cover 34, which is a headed cylinder, covers the upper plate-shaped yoke 3.
The upper plate-shaped yoke 31 is fixed to the outer periphery of the hole 1 with a bolt 35, and the adjustment bolt 36 screwed into the center part.
The upper plate-shaped yoke 31 is placed on the upper end of the cylindrical yoke 33 and can be slightly moved vertically by screwing the adjustment bolt 36 back and forth. It is configured such that the distance between the cover 34 and the columnar yoke 33 can be adjusted by fixing bolts 37 provided around the adjustment bolts 36.
It is a configuration that can be fixed.

上記の上下の板状継鉄31,32の対向面に、
中心に孔部を有する円板継鉄38,39を介して
着設される永久磁石構成体40,50は、中央部
永久磁石41,51と外周部永久磁石43,53
からなり、中央部永久磁石41,51が、その中
心に磁力調整用孔部42,52を設けた8角形板
状に形成され、8個の略台形板状の外周部永久磁
石43,53が、中央部永久磁石41,51の各
辺に当接させ、かつ台形楔状継鉄44,54を介
して傾斜させて、凹状の対向面を形成するよう周
設してある。
On the opposing surfaces of the upper and lower plate yokes 31 and 32,
Permanent magnet structures 40, 50 are attached via disk yokes 38, 39 having holes in the center, and include central permanent magnets 41, 51 and outer peripheral permanent magnets 43, 53.
The central permanent magnets 41, 51 are formed into an octagonal plate shape with magnetic force adjustment holes 42, 52 provided in the center, and eight approximately trapezoidal plate-shaped outer peripheral permanent magnets 43, 53 are formed. , are in contact with each side of the central permanent magnets 41, 51, and are provided around the periphery so as to form concave opposing surfaces by being inclined through trapezoidal wedge-shaped yokes 44, 54.

また、永久磁石構成体40,50は、ブロツク
状のFe−B−R系永久磁石を多数個用いて、着
磁組立にて前記形状に構成し、磁極面に対して垂
直方向に磁化方向を有している。
The permanent magnet structures 40 and 50 are constructed into the above shape by magnetizing and assembling a large number of block-shaped Fe-BR permanent magnets, and the magnetization direction is perpendicular to the magnetic pole surface. have.

凹状磁極面を形成して対向する永久磁石構成体
40,50には、それぞれ前述した第5図と同構
成からなる、すなわち、8角形の平面部の外周に
周設した8個の台状形傾斜部を周設し、さらに、
対向平面部に円形突起部46,56を有する断面
が略凹状湾曲面からなる磁極片45,55が着設
してあり、一対の磁極片45,55間に形成され
る空隙60に、磁束を効率よく集束させる機能を
有する。
The permanent magnet structures 40 and 50 facing each other with concave magnetic pole surfaces each have the same structure as in FIG. A sloped portion is provided around the circumference, and further,
Magnetic pole pieces 45 and 55 having circular protrusions 46 and 56 on opposing plane parts and having curved surfaces with a substantially concave cross section are attached, and a magnetic flux is directed into the air gap 60 formed between the pair of magnetic pole pieces 45 and 55. It has the function of efficiently focusing.

板状継鉄31,32の非着設側面の中央部に
は、所謂テーパー状の孔部70,71が設けら
れ、円板継鉄38,39の孔部に連通し、中央部
永久磁石41,51の磁力調整用孔部42,52
へ嵌入させる円柱状磁性材からなる磁力調整材7
2が、嵌入量調整可能に円板継鉄38,39の孔
部周囲に着設してある。
So-called tapered holes 70, 71 are provided in the center of the non-attached side surfaces of the plate yokes 31, 32, which communicate with the holes of the disk yokes 38, 39, and are connected to the center permanent magnet 41. , 51 magnetic force adjustment holes 42, 52
Magnetic force adjustment material 7 made of a cylindrical magnetic material to be inserted into
2 are installed around the holes of the disc yokes 38 and 39 so that the amount of insertion can be adjusted.

板状継鉄31,32のテーパー状孔部70,7
1は、板状継鉄31,32の中央部の磁束量が少
なくなることに着目し、継鉄の重量削減と、前記
磁力調整材72が外部に露出するのを避ける目的
で配置してある。
Tapered hole portions 70, 7 of plate yokes 31, 32
1 is arranged to reduce the weight of the yoke and to prevent the magnetic force adjustment material 72 from being exposed to the outside, focusing on the fact that the amount of magnetic flux in the center of the plate yokes 31 and 32 is reduced. .

また、磁界の均一度、分布等の調整は、前述の
永久磁石構成体40,50の対向距離を調整する
柱状継鉄33上端に当接する調整用ボルト36
と、永久磁石構成体40,50の中心部に嵌入し
て、中央部永久磁石41,51からの磁束短絡量
を調整する磁界調整材72のほか、円板継鉄3
8,39を水平方向に押圧微動させて行なつた
り、その厚み等により永久磁石構成体40,50
のレベリングを行なうこともでき各手段を適宜選
定するとよい。
Further, the uniformity, distribution, etc. of the magnetic field can be adjusted using the adjusting bolt 36 that comes into contact with the upper end of the columnar yoke 33 that adjusts the facing distance between the permanent magnet structures 40 and 50.
In addition to the magnetic field adjustment material 72 that fits into the center of the permanent magnet structures 40 and 50 and adjusts the amount of magnetic flux short circuit from the central permanent magnets 41 and 51, the disc yoke 3
8, 39 in the horizontal direction, or by slightly moving the permanent magnet structures 40, 50 depending on their thickness, etc.
It is also possible to carry out leveling, and each means may be selected appropriately.

さらに円板継鉄38,39と楔状継鉄44,5
4を一体に形成してもよい。
Furthermore, disc yokes 38, 39 and wedge-shaped yokes 44, 5
4 may be integrally formed.

上記構成からなる磁気回路において、永久磁石
構成体40,50から発生する磁束は、磁極片4
5,55を介して磁石の磁化方向と同一方向に収
束されて磁界形成するため、漏洩磁束が減少し、
空隙60内には極めて高い均一度を有する静磁界
が得られる。
In the magnetic circuit having the above configuration, the magnetic flux generated from the permanent magnet components 40 and 50 is transmitted to the magnetic pole piece 4.
5 and 55 to form a magnetic field converged in the same direction as the magnetization direction of the magnet, leakage magnetic flux is reduced,
A static magnetic field with extremely high uniformity is obtained within the air gap 60.

特に、凹状の磁極面を形成した永久磁石構成体
40,50に、深皿状の磁極片45,55を着設
した構成であるため、磁極片45,55の外周面
積が、第6図に示す環状突起5を有する磁極片2
の外周面積より、小さくなり、漏洩磁束が著しく
減少する効果を有する。
In particular, since the permanent magnet components 40, 50 each having a concave magnetic pole surface are provided with deep dish-shaped magnetic pole pieces 45, 55, the outer circumferential area of the magnetic pole pieces 45, 55 is as shown in FIG. A magnetic pole piece 2 with an annular protrusion 5 shown
This has the effect of significantly reducing leakage magnetic flux.

ちなみに、第1図に示した構成のNMR−CT
に、最大エネルギー積35MGO8の特定を有する
Fe−B−R系永久磁石を用い、磁極片の対向距
離として、570mmを設定して組立を行なつたとこ
ろ、空隙中央部での磁界強度は1.5kGであり、
300mmDSV内で、40ppm以下の均一磁界を得るこ
とができ、永久磁石構成体の重量は1.1トンであ
つた。
By the way, NMR-CT with the configuration shown in Figure 1
has a maximum energy product of 35MGO 8 specific
When assembling Fe-BR-based permanent magnets and setting the facing distance of the magnetic pole pieces to 570 mm, the magnetic field strength at the center of the air gap was 1.5 kG.
A uniform magnetic field of less than 40 ppm could be obtained within 300 mm DSV, and the weight of the permanent magnet structure was 1.1 tons.

また、同等組成、磁気特性の永久磁石用いて、
第6図に示す構成からなる従来磁気回路にて、上
記のこの発明の実施例と同程度の均一磁界範囲及
び磁界強度を得るには、1.5トンの永久磁石を必
要とした。
In addition, using permanent magnets with the same composition and magnetic properties,
In the conventional magnetic circuit having the configuration shown in FIG. 6, a permanent magnet of 1.5 tons was required to obtain a uniform magnetic field range and magnetic field strength comparable to that of the embodiment of the present invention described above.

さらに、永久磁石の継鉄当接面を透過する磁束
量φ1と空隙中央部、すなわち磁極片の中央平面
間の空間に集束される磁束量0φ2とを測定し、磁
束利用率(φ1/φ2×100%)を比較したところ、 本発明磁気回路(第1図)の磁束利用率=45% 従来磁気回路(第6図)の磁束利用率=32%の
結果を得た。この発明による磁気回路が、漏洩磁
束が少なく、著しく磁気効率が高いことが分る。
Furthermore, we measured the amount of magnetic flux φ 1 that passes through the yoke contact surface of the permanent magnet and the amount of magnetic flux 0 φ 2 that is concentrated in the center of the air gap, that is, the space between the center planes of the magnetic pole pieces, and calculated the magnetic flux utilization rate (φ 12 ×100%), it was found that the magnetic flux utilization rate of the magnetic circuit of the present invention (FIG. 1) was 45%, and the magnetic flux utilization rate of the conventional magnetic circuit (FIG. 6) was 32%. It can be seen that the magnetic circuit according to the present invention has low leakage magnetic flux and extremely high magnetic efficiency.

【図面の簡単な説明】[Brief explanation of drawings]

第1図はこの発明による磁界発生装置に用いる
磁気回路の横断上面図とB−B断面図である。第
2図から第4図は磁気回路の継鉄を示す斜視説明
図である。第5図はこの発明による磁気回路の磁
極片を示す断面図と底面図並びに他の磁極片の断
面図である。第6図は従来の磁気回路を示す縦断
説明図である。 10,14,18,30……継鉄、31,32
……板状継鉄、33……円柱状継鉄、34……カ
バー、35……ボルト、36……調整用ボルト、
37……固定ボルト、38,39……円板継鉄、
40,50……永久磁石構成体、42,52……
テーパー状孔部、43,53……外周部永久磁
石、44,54……楔状継鉄、45,55……磁
極片、46,56……突起部、60……空隙、7
0,71……テーパー状孔部、72……磁界調整
材。
FIG. 1 is a cross-sectional top view and a BB sectional view of a magnetic circuit used in a magnetic field generating device according to the present invention. 2 to 4 are perspective explanatory views showing the yoke of the magnetic circuit. FIG. 5 is a cross-sectional view and a bottom view showing a magnetic pole piece of a magnetic circuit according to the present invention, as well as a cross-sectional view of another magnetic pole piece. FIG. 6 is a longitudinal sectional view showing a conventional magnetic circuit. 10, 14, 18, 30... Yoke, 31, 32
... Plate-shaped yoke, 33 ... Cylindrical yoke, 34 ... Cover, 35 ... Bolt, 36 ... Adjustment bolt,
37... Fixing bolt, 38, 39... Disc yoke,
40,50...Permanent magnet structure, 42,52...
Tapered hole, 43, 53... Permanent magnet at outer periphery, 44, 54... Wedge-shaped yoke, 45, 55... Magnetic pole piece, 46, 56... Protrusion, 60... Gap, 7
0, 71...Tapered hole portion, 72...Magnetic field adjustment material.

Claims (1)

【特許請求の範囲】[Claims] 1 空隙を形成して対向する一対の永久磁石構成
体を継鉄で磁気的結合し、各永久磁石構成体の空
隙対向面に磁極片を固着し、該空隙に磁界を発生
させる磁界発生装置において、平板状の中央部永
久磁石と、中央永久磁石の外周部に傾斜させて周
設または周配置する外周部永久磁石とにより、磁
極面に垂直方向に磁化された各対の永久磁石磁極
面が、空隙に対して凹状湾曲面を形成したことを
特徴とする磁界発生装置。
1. In a magnetic field generating device that magnetically couples a pair of permanent magnet structures facing each other with an air gap formed therein using a yoke, fixes a magnetic pole piece to the air gap facing surface of each permanent magnet structure, and generates a magnetic field in the air gap. , the magnetic pole surface of each pair of permanent magnets is magnetized perpendicularly to the magnetic pole surface by the flat central permanent magnet and the peripheral permanent magnet installed or arranged around the central permanent magnet in an inclined manner. , A magnetic field generating device characterized in that a concave curved surface is formed with respect to the air gap.
JP61099938A 1985-12-27 1986-04-30 Magnetic field generating equipment Granted JPS62256416A (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP61099938A JPS62256416A (en) 1986-04-30 1986-04-30 Magnetic field generating equipment
US06/909,327 US4679022A (en) 1985-12-27 1986-09-19 Magnetic field generating device for NMR-CT
EP86307272A EP0228154B1 (en) 1985-12-27 1986-09-22 Magnetic field generating device for nmr-ct
DE8686307272T DE3676066D1 (en) 1985-12-27 1986-09-22 DEVICE FOR GENERATING MAGNETIC FIELDS FOR MAGNETIC NUCLEAR RESONANCE TOMOGRAPHY.

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61099938A JPS62256416A (en) 1986-04-30 1986-04-30 Magnetic field generating equipment

Publications (2)

Publication Number Publication Date
JPS62256416A JPS62256416A (en) 1987-11-09
JPH0320053B2 true JPH0320053B2 (en) 1991-03-18

Family

ID=14260656

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61099938A Granted JPS62256416A (en) 1985-12-27 1986-04-30 Magnetic field generating equipment

Country Status (1)

Country Link
JP (1) JPS62256416A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2953659B1 (en) 1998-08-06 1999-09-27 住友特殊金属株式会社 Magnetic field generator for MRI, method of assembling the same, and method of assembling magnet unit used therein
JP4813645B2 (en) * 1999-11-16 2011-11-09 日立金属株式会社 Magnetic pole unit, method for assembling the same, and magnetic field generator
JP4617596B2 (en) * 2001-04-24 2011-01-26 日立金属株式会社 MRI magnetic field generator and MRI apparatus using the same
JP2004349276A (en) * 2003-04-25 2004-12-09 Japan Science & Technology Agency Superconducting permanent magnet device
JP5224275B2 (en) * 2008-03-28 2013-07-03 日立金属株式会社 PET / MRI integrated device
WO2013114993A1 (en) * 2012-01-30 2013-08-08 三菱電機株式会社 Magnetic circuit

Also Published As

Publication number Publication date
JPS62256416A (en) 1987-11-09

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